The Width of a Solar Coronal Mass Ejection and the Source of the Driving Magnetic Explosion: A Test of the Standard Scenario for CME Production

We show that the strength (Snare) of the magnetic field in the area covered by the flare arcade following a CME-producing ejective solar eruption can be estimated from the final angular width (Final theta sub(CME)) of the CME in the outer corona and the final angular width ( theta sub(Flare)) of the...

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Bibliographic Details
Published in:The Astrophysical journal 2007-10, Vol.668 (2), p.1221-1231
Main Authors: Moore, Ronald L, Sterling, Alphonse C, Suess, Steven T
Format: Article
Language:English
Subjects:
Astronomy
Earth, ocean, space
Exact sciences and technology
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Summary:We show that the strength (Snare) of the magnetic field in the area covered by the flare arcade following a CME-producing ejective solar eruption can be estimated from the final angular width (Final theta sub(CME)) of the CME in the outer corona and the final angular width ( theta sub(Flare)) of the flare arcade: B sub(Flare) approximately 1.4 [(Final theta sub(CME))/ theta sub(Flare)] super(2) G. We assume (1) the flux-rope plasmold ejected from the flare site becomes the Interior of the CME plasmold; (2) in the outer corona (R > 2 R [unk]) the CME is roughly a "spherical plasmold with legs" shaped like a lightbulb; and (3) beyond some height in or below the outer corona the CME plasmold is in lateral pressure balance with the surrounding magnetic field. The strength of the nearly radial magnetic field in the outer corona is estimated from the radial component of the Interplanetary magnetic field measured by Ulysses. We apply this model to three well-observed CMEs that exploded from flare regions of extremely different size and magnetic setting. One of these CMEs was an over-and-out CME, that is, in the outer corona the CME was laterally far offset from the flare-marked source of the driving magnetic explosion. In each event, the estimated source-region field strength Is appropriate for the magnetic setting of the flare. This agreement (1) indicates that CMEs are propelled by the magnetic field of the CME plasmold pushing against the surrounding magnetic field; (2) supports the magnetic-arch-blowout scenario for over-and-out CMEs; and (3) shows that a CME's final angular width in the outer corona can be estimated from the amount of magnetic flux covered by the source-region flare arcade.
ISSN:0004-637X
1538-4357
DOI:10.1086/521215